1 / 22

Pattern Formations with a Zooplankton: Experiment and Theory

Pattern Formations with a Zooplankton: Experiment and Theory. Anke Ordemann Frank Moss. Support:. US Office of Naval Research Alexander von Humboldt Foundation. Motivation: Vortex-swarming of ‘self-propelled’ animals. Blue Planet: Seas of Life, Discovery Channel 2001. Outline.

zenia-chaney
Download Presentation

Pattern Formations with a Zooplankton: Experiment and Theory

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Pattern Formations with a Zooplankton: Experiment and Theory Anke Ordemann Frank Moss Support: US Office of Naval Research Alexander von Humboldt Foundation

  2. Motivation:Vortex-swarming of ‘self-propelled’ animals Blue Planet: Seas of Life, Discovery Channel 2001

  3. Outline • The Active Brownian Particle (ABP) Theory – Erdmann, Ebeling, Schweitzer – Humboldt University Berlin • Single (few) Particle Motions & Bifurcations • About Daphnia – the experiment • Random Walk Theory - Measures and Results • Symmetry Breaking – Vortex motion • Simulation using RWT • Summary

  4. Active Brownian Particle (ABP)with internal energy depot [Schweitzer et al., PRL 80, 5044 (1998)] Energy depot: space-dependent take-up q(r), internal dissipation ce(t), conversion of internal energy into kinetic energy d2e(t)v2 (For uniform distr: q(r) = q0) A velocity dependent dissipation

  5. Hopf bifurcation: Fixed point  limit cycle pair Bifurcation parameter:

  6. Daphnia make vortices Side view of vortex-swarming zooplankton Daphnia in our lab. Picture by D.F. Russell.  Schlieren technique movie of Daphnia motion by Ai Nihongi and Rudi Strickler. 

  7. About Daphnia Daphnia magna, common “water flea”. • They are: • Attracted to visible light (VIS) • Repelled by ultra violet (not used here) • Blind to infra red (IR) Record their motions using IR and manipulate motions using VIS

  8. Apparatus • Side and bottom views recorded simultaneously • VIS light shaft is the cue • Illumination and recording in IR

  9. Example RecordingsAbout 40 animals, approximately equal numbers circling in opposite directions Bottom view of a few Daphnia moving around light shaft (radius r =5mm). Movie is speeded up 4 times. Five successive positions of Daphnia taken in intervals of 0.3s (black/white inverted).

  10. Observation of a single Daphnia Note reversal X(t) Y(t) Bottom view of individual Daphnia moving around light shaft. Movie is speeded up 3 times. Track of one Daphnia individually circling horizontally around light shaft (146s). Single Daphnia circle individually in both directions around light shaft, frequently changing direction

  11. How to characterize observed circular motion?- M=624 moves from 4 different animals - Average speed vavg = 5.71 ± 1.35 mm/s MC= Number of successive moves before changing direction (CCW vvs CW). MC  = 11.8

  12. Random Walk Theory - but needMotion of single Daphnia in the dark. 1599 moves from 8 different animals Example track, 200 hops  X Distribution of turning angles, = directional change after each hop  Y P() symmetric about 0. ||  35 (Similar to oceanic copepods)

  13. Random Walk Theory *Short range temporal correlation *Attraction to light • Daphnia in darkness: At the end of each step, the direction of next time step at ti+1 is randomly chosen from observed distribution of turning angle (DTA) • Daphnia in light field: At the end of each time step, the direction is again chosen from the DTA, but an additional kick of strength r*L/(L-1) towards the light (parabolic potential) is added and the final heading is rescaled to unit length. [0  L< 1]

  14. Results of the Simulation for various L: P(θ) Heading angle,  P(r) Radius, r

  15. Results (cont) MC L P(MC) L = 0.4 MC

  16. Many Particle Generalizations - ABP (Humboldt) Particle-Particle attractive interaction  Mean field potential (ABP) and probability densities of the limit cycle motions. Symmetric pair of limit cycles. Interacting Active Brownian Particles[Schweitzer et al., PRE 64, 021110 (2001); Ebeling and Schweitzer, Theory Biosci. 120, 20 (2001); Erdmann et al., PRE 65, 061106 (2002)]

  17. Many Particle Generalizations – Levine Short range repulsion and long range attraction added to the model of Self-Propelled Interacting Particles [Levine et al., PRE 63, 017101 (2001)] Self propelling force, (no alignment) Self propelling force, (with alignment – range lc)

  18. Transition to Vortex Motion by a Daphnia SwarmModels:Symmetry of limit cycles must be broken.Velocity alignment; Avoidance Daphnia experiment:hydrodynamic coupling likely(for birds and fish the alignment is visual with neighbors) CCW Motion and spiral arms

  19. Another example CW Motion (after a time delay)

  20. RWT Simulation of the transition: Interacting RW with DTA • Simple model for (vortex-) swarming Daphnia • Indirect inter-agent interactions via water drag are incorporated by adding ‘alignment’ or ‘water drag’ kick proportional to: A local order parameter: Ntot = 30 O Time, t Global order parameter: O = (NCW  NCCW )/Ntot

  21. Conclusions Theory predicts four motions: • Noisy fixed point • Symmetric pair of limit cycles • Swarming • Transition to vortex All four motions can be observed in experiments with Daphnia

  22. Discussion What are the minimum ingredients that lead to these motions? A. Few animal (low density) experiments: • Self-propelled particles (finite non-zero velocity) • Assigned preference to move in ‘forward’ direction • Confinement, arising from Attraction (either as mean field potential from interagent interactions or as external attractive potential) B. Large animal density experiments: • In addition to the above – a symmetry breaking (velocity alignment) mechanism.

More Related